Field-effect transistor

ABSTRACT

A field-effect transistor (10, FIG. 2) possesses improved electrostatic discharge characteristics. The transistor (10), formed in a p-type semiconductor substrate, comprises a gate (16) that forms a channel between two adjacent n-regions (12 and 14). At least one of the n-regions (12) has an n-well (22) below and centered about a contact pad (18). The n-well (22) has a second lower concentration of n-type impurities than either of the n-regions.

This is a continuation of application Ser. No. 08/226,238 filed Apr. 11, 1994 now U.S. Pat. No. 5,714,783.

TECHNICAL FIELD OF THE INVENTION

This invention relates to integrated circuits, and more particularly to a field-effect transistor.

BACKGROUND OF THE INVENTION

Integrated circuits are vulnerable to a phenomenon generically referred to as electrostatic discharge ("ESD"). During handling, integrated circuits can build up relatively large static charges on their inputs. These charges, if not properly compensated for, may flow or "discharge" to a lower potential region. Discharging in this way produces large electric fields within the transistors that are immediately connected to the various inputs and outputs of a particular circuit. High electric fields in turn, produce high temperature gradients and ultimately yield thermal electrode migration ("TEM") within the transistor. TEM describes how a transistor fails when the contact to a doped source/drain region separates from the region. TEM causes irreversible circuit failures. ESD and TEM become more severe as circuits dimensions decrease. The smaller the dimension of, for instance, a doped drain region, the higher the electric field will be per charge. As a result, new semiconductor technologies require more effective designs to overcome these problems.

Heretofore, electronics designers have relied on the inherent diode existing between the source/drain region and the grounded substrate of a NMOS FET or of a n-channel FET in a CMOS transistor pair. The p-n junction in such a transistor protects the contact from up to 18 volts of charge buildup. After approximately that amount of buildup, however, ESD occurs from the drain to the ground plane through the substrate. Some designs modify certain characteristics of the drain to improve ESD performance. In particular, in some transistors may increase the distance between the affected contact and the gate. This modification increases the ESD protection up to a distance of approximately 6 μm. Beyond 6 μm, however, the ESD performance flattens and ultimately decreases as electrostatic charge shorts to the p substrate material at a different point. Such a transistor also suffers from lower gain as the larger source-drain region increases resistivity. Other designers simply increase the volume of the n drain to increase the area of the drain-substrate interface. Unfortunately, this also increases the resistance and capacitance of the transistor. The transistor, therefore, suffers from a lower gain and a lower maximum switching speed.

Therefore, a need exists for a transistor having a greater breakdown voltage between the source-drain regions and the corresponding p substrate with no loss of switch performance.

SUMMARY OF THE INVENTION

In accordance with the present invention, a field-effect transistor is provided which substantially eliminates and prevents the above disadvantages and problems associated with prior transistors.

The transistor of the present invention is formed in a p-type semiconductor substrate and comprises a gate that forms a channel between two adjacent n-regions. At least one of the n-regions has an n-well below and centered about a contact pad. The n-well has a second lower concentration of n-type impurities than either of the n-regions.

The present invention provides numerous technical advantages over prior transistors. A transistor constructed according to the present invention exhibits a greater breakdown voltage between n-doped regions and the related p substrate. This substantially improves the device's electrostatic discharge or ESD performance.

Additionally, the disclosed transistor minimizes system resistance and capacitance to permit faster transistor switching speeds.

BRIEF DESCRIPTION OF THE DRAWINGS

For a more complete understanding of the present invention and the advantages thereof, reference is now made to the following description taken in conjunction with the accompanying drawings in which:

FIG. 1 depicts in planar view a transistor made according to the preferred embodiment of the present invention;

FIG. 2 depicts a cross sectional view taken along line 2--2 of FIG. 1;

FIG. 3 depicts in planar view a transistor according to an alternative embodiment of the present invention; and

FIG. 4 depicts a cross sectional view taken along line 4--4 of FIG. 3.

DETAILED DESCRIPTION OF THE INVENTION

The preferred embodiment of the present invention and its advantages are best understood by referring to FIGS. 1 through 4 of the drawings, like numerals being used for like and corresponding parts of the various drawings.

FIG. 1 depicts generally a planar view of a metal oxide semiconductor field-effect transistor 10 ("MOSFET") wherein a second n region provides improved ESD performance. MOSFET 10 is an NMOS transistor or a n-channel transistor of a CMOS transistor pair. MOSFET 10 has a first n-type source-drain region 12 and a second n-type source-drain region 14. Each region is either doped or implanted into a p-type substrate. An insulator (depicted in FIG. 2) separates metal gate 16 from the underlying p-substrate. Contact pads 18 and 20 supply or remove electric current from doped regions 12 and 14 respectively. Pads 18 and 20 are typically exposed subregions of regions 12 and 14 and permit an ohmic contact to other components (not depicted). First source-drain region 12 also contains an n-well 22 below each of the contact pads 18. As will be described below, each n-well 22 increases the ESD performance of MOSFET 10.

Metal gate 16 controls the flow of current between regions 12 and 14 by creating an electric field between the two regions. An electric field causes a channel to form in the substrate between regions 12 and 14 and below the gate insulating layer.

FIG. 2 depicts a cross-sectional view of MOSFET 10 along line 2--2 of FIG. 1 that shows the vertical integration of n-well 22 and first source-drain region 12. In addition, insulating layer 24 separates gate 16 from substrate 26. Substrate 26 includes a p-type semiconductor material, while regions 12 and 14 are heavily doped ("n+") with n-type impurities. A lower concentration of n-type impurities than either region 12 or 14 dopes n-well 22.

Transistor 10 naturally forms two p-n junctions that act as diodes. One of these, the junction between region 12 and substrate 26, may act as a barrier to the discharge of positive electrostatic charge from contact 18 to the ground plane through substrate 26. ESD from contact 20 is not a concern for positive polarity stress since, region 14 electrically connects to substrate 26 through the ground plane. Also, it is not a concern for negative polarity stress for grounded substrate technologies. However, the barrier between region 12 and substrate 26 limits the ESD characteristics of region 12 in previous transistors. In particular, source-drain region 12 must have a low resistance and low capacitance in these transistors. These requirements lead to the constraints of small size and high concentrations of n-type carriers. Small size, however, causes large temperature gradients across the region and makes the transistor more susceptible to thermal electrode migration or TEM. A high dopant concentration in region 12 causes a relatively low breakdown voltage between region 12 and substrate 26. For example, charge flows between region 12 and substrate 26 when a voltage difference of 18 volts develops between the two regions. Typically, the concentration of n carriers is 10¹⁹ atoms/cm³ in regions 12 and 14.

According to the preferred embodiment, a well of lightly doped n-type carriers below contact 18 in region 12 improves ESD performance without substantially increasing system resistance or capacitance. Lightly doping a region below contact 18, increases the breakdown voltage between region 12 and substrate 26 to between 40 and 50 volts. This breakdown voltage increase gives the transistor the breakdown voltage of a lightly doped p-n junction and does not depend on the size of n-well 22. The size of the contact pad 18 limits the size of n-well 22. The footprint of the n-well should be generally the same size or larger than the footprint of the contact pad 18. Present semiconductor processes, however, may fabricate contact pads 18 substantially smaller than n-well 22. In particular, present technology limits the size of n-well 22 to approximately 6×6 μm², while contact pad 18 may be approximately 1.5×1.5 μm². N-well 22 must extend below the bottom of the overlying source-drain region 12. N-well 22 preferably extends to a total depth of five to seven times the depth of region 12. N-well 22 within region 18 has little or no effect on the performance of MOSFET 10. The depth of n-well 22 therefore ranges from 1 to 2 μm for typical 0.5 μm processes.

Transistor 10 may be fabricated from a combination of photolithographic processes according to known methods.

EXAMPLE

Transistor 10 begins with a p-type semiconductor substrate, preferably a p-type silicon substrate 26. Substrate 26 is then masked such that only the surface of substrate 26 below regions 28 and 30 is exposed. Field oxide regions 28 and 30 are formed in accordance with well-known processes utilized to prove device-to-device isolation. In particular, regions 28 and 30 may be formed by the local-oxidation-of-silicon ("LOCOS") or the poly-buffered LOCOS process ("PBL"). The remaining photoresist mask is then removed.

Insulating layer 24 is formed using the same techniques as regions 28 and 30. The resulting component is first masked with photoresist to expose only the surface of substrate 26 where layer 24 is to be grown. The entire workpiece is covered with 5,000 to 10,000 Angstroms of aluminum to form gate 16. The unwanted aluminum will be removed with the underlying photoresist layer when the resist layer is removed.

The substrate at this point then acts as a self-aligned implant mask for regions 12 and 14. The heavily doped source-drain regions 12 and 14 are implanted with an n-type species such as arsenic, phosphorus, or antimony. Here the implantation is performed at 100 keV at a dose of 1E15 atoms/cm². Following the implantation, a rapid thermal anneal ("RTA") or furnace anneal process is performed. The RTA process is preferably performed at 1,000° C. for 30 seconds. Furnace annealing may be instead used at, for instance, 900° C. for one hour. The resulting n+ regions are approximately 0.5 μm deep and have a resistivity of approximately 25 to 30 ohms/sq.

A third mask is then applied to obscure all of region 12 except the central area around the future site of each contact pad. A lighter dose of the same species is then implanted to form n-well 22 to a depth of approximately 1 micron. The second implantation step may be accomplished with an implant energy of 150 keV and a dose of 1E13 atoms/cm². This results in an n-type region having a resistivity of approximately 1500 Ohms/sq. The third photoresist layer may then be removed.

FET 10 is completed by applying another mask, exposing contact pads 18 on regions 12 and 14, depositing an interconnect layer, and patterning the layer to connect FET 10 to other elements on substrate 26.

FIGS. 3 and 4 depict a second embodiment of the disclosed invention for use with floating substrate technology MOSFETs. NMOS FET 32 differs from the transistor depicted in FIGS. 1 and 2 in that source drain region 14 is not connected to substrate 26. Electrostatic discharge may therefore occur under certain circumstances between second region 14 and substrate 26 for negative polarity stress. In such a case, it is advantageous to place a second n-well 34 to protect transistor 32 more completely. N-well 34 is constructed using the same techniques as described above.

Although the disclosed invention is described in connection with an abrupt junction thick-field NMOS FET, its scope should not be limited to such devices. The disclosed invention is applicable to other technologies including those transistors fabricated with lightly doped drains, double diffused drains and with thin oxide or polysilicon gate transistors.

Moreover, although the present invention and its advantages have been described in detail, it should be understood that various changes, substitutions and alterations can be made herein without departing from the spirit and scope of the invention as defined by the appended claims. 

What is claimed is:
 1. A semiconductor device comprising:a substrate having a first conductivity type; an insulating layer formed adjacent a first surface of the substrate; a gate disposed adjacent the insulating layer; first and second doped regions formed within the substrate, the first and second doped regions each having an edge adjacent the gate and the substrate and each having a first doping concentration of a second conductivity type, the second conductivity type being opposite the first conductivity type, the first and second doped regions each extending into the substrate to a first depth; a third doped region of the second conductivity type formed within the substrate, the third doped region extending into the substrate to a second depth, the second depth being greater than the first depth, the third doped region having a doping concentration less than the first doping concentration; and a first conductor directly contacting the first doped region only within a perimeter of the first doped region and within a perimeter of the third doped region.
 2. The device of claim 1 and further comprising:a fourth doped region extending into the substrate to the second depth, the fourth doped region having a doping concentration less than the first doping concentration; and a second conductor directly contacting the second doped region only within a perimeter of the second doped region and within a perimeter of the fourth doped region.
 3. The device of claim 1 wherein the first conductivity type is p-type.
 4. The device of claim 1 wherein the semiconductor device comprises a field effect transistor and wherein the first and second doped regions comprise source-drain regions.
 5. The device of claim 1 wherein the second depth is five to seven times greater than the first depth.
 6. The device of claim 1 wherein the substrate comprises silicon and the gate comprises polycrystalline silicon.
 7. The device of claim 1, wherein the first and second doped regions are doped with arsenic dopants.
 8. The device of claim 1 and further comprising field insulation regions adjacent the first and second doped regions.
 9. The device of claim 8 wherein the gate comprises aluminum.
 10. The device of claim 1 wherein the gate comprises a metal.
 11. The device of claim 1, wherein each of the first and second doped regions comprise a double diffused region formed in the substrate.
 12. A semiconductor device comprising:a substrate having a surface of a first conductivity type; an insulating layer overlying the surface of the substrate; a first elongated doped region formed at the surface of the substrate, the first elongated doped region having a first edge adjacent the substrate, the first elongated doped region having a first doping concentration of a second conductivity type, the second conductivity type being opposite the first conductivity type, the first doped region extending into the substrate to a first depth; a second elongated doped region formed at the surface of the substrate, the second elongated doped region having a second edge formed parallel to and spaced apart from the first edge, the second elongated doped region having the first doping concentration of the second conductivity type, the second doped region extending into the substrate to the first depth; a current path within the substrate between the first and second edges; a third doped region having a second doping concentration of the second conductivity type formed within the substrate, the third doped region extending into the substrate to a second depth, the second depth being greater than the first depth, the second doping concentration being less than the first doping concentration; and a first conductor directly contacting the first elongated doped region only within a perimeter of the first elongated doped region and within a perimeter of the third doped region.
 13. A device as in claim 12, wherein the first conductor comprises a plurality of conductive regions disposed linearly and parallel to the first edge.
 14. A device as in claim 12, further comprising:a fourth doped region having the second doping concentration of the second conductivity type, the fourth doped region extending into the substrate to the second depth; and a second conductor directly contacting the second doped region only within a perimeter of the second doped region and within a perimeter of the fourth doped region.
 15. A device as in claim 14, wherein each of the first and second conductors comprise a plurality of conductive regions disposed linearly and parallel to the first edge.
 16. A device as in claim 15, further comprising field insulation regions adjacent the first and second doped regions.
 17. A device as in claim 16, wherein the first and second elongated doped regions are lightly doped source-drain regions of a field effect transistor.
 18. A device as in claim 16, wherein the first and second elongated doped regions are double diffused source-drain regions of a field effect transistor.
 19. A device as in claim 16, wherein the gate is polycrystalline silicon.
 20. A device as in claim 12, wherein the first conductivity type is p-type.
 21. A device as in claim 12, further comprising a gate overlying the current path.
 22. The device of claim 12 wherein the second depth is five to seven times greater than the first depth. 